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Proof of Scaled Cutoffs and the Second-Moment Test Functions: Uniform Derivative Bounds and Agreement on a Ball

lemmalem:cutoff-second-moment-test-functions-2026a
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· 11,418 chars · 28 deps · depth 20 Reason: Goal 3C Batch A: proof via the scaling substitution and the product rule.

The cutoff is a scaling substitution of the bump function, so its partial derivatives are the rescaled partial derivatives of the bump, which are bounded because they are continuous with compact support; the product rule then gives the derivatives of the second-moment test functions, which are estimated on the ball of radius 2R and vanish outside it.

Proof

Each result cited is universally quantified over the data in its own statement. Write ι\iota for the canonical map of The Canonical Map from the Natural Numbers to a Field, πl:RqR\pi_{l}:\mathbb{R}^{q}\to\mathbb{R}, πl(x)=xl\pi_{l}(x)=x_{l}, for the coordinate functions, and W2={yRq:y>2}W_{2}=\{y\in\mathbb{R}^{q}:\lVert y\rVert>2\}. Continuity of a function on Rq\mathbb{R}^{q} is that of Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §extrema; by claim 1 of Euclidean Continuity Agrees with Metric Continuity for Real-Valued Functions it agrees with continuity at every point in the sense of Continuity at a Point for Maps Between Euclidean Spaces, which is the notion used in C^k Maps on a Euclidean Open Set. A function of class Ck+1C^{k+1} is of class C1C^{1} and its partial derivatives are of class CkC^{k}, by clause 2 of C^k Maps on a Euclidean Open Set; a smooth function is of class CkC^{k} for every kk (Smooth Map on a Euclidean Open Set), so its partial derivatives are smooth as well. A function of class C1C^{1} is continuous with continuous partial derivatives, by clause 1 of C^k Maps on a Euclidean Open Set.

For points y,yRqy,y'\in\mathbb{R}^{q} we use y=y+(yy)y=y'+(y-y') and yy=yy\lVert y-y'\rVert=\lVert y'-y\rVert (claims 2 and 3 of Euclidean Space Rn\mathbb{R}^n is a Real Vector Space, and claim 5 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n with λ=1\lambda=-1), together with dE(y,y)=yyd_{E}(y,y')=\lVert y-y'\rVert (claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n).

Step 0: the derivatives of χ\chi are bounded and vanish on W2W_{2}. The set W2W_{2} is open: if yW2y\in W_{2} and yy<y2\lVert y'-y\rVert<\lVert y\rVert-2, then yy+yy\lVert y\rVert\le\lVert y'\rVert+\lVert y-y'\rVert by claim 6 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n applied to y=y+(yy)y=y'+(y-y'), so y>2\lVert y'\rVert>2; this says that the open ball of centre yy and radius y2\lVert y\rVert-2 lies in W2W_{2}, so W2W_{2} is open in the metric sense, hence open by Euclidean Openness Agrees with Metric Openness on Rn\mathbb{R}^n. Let u:RqRu:\mathbb{R}^{q}\to\mathbb{R} be of class C1C^{1} with u=0u=0 on W2W_{2} and let l[q]l\in[q]. Then uW2=0uW2u|_{W_{2}}=0\cdot u|_{W_{2}} is of class C1C^{1} on W2W_{2} by claim 3 of Restriction of a CkC^k Map to an Open Subset, so by the scalar-multiple rule of claim 1 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set, l(uW2)=0l(uW2)=0\partial_{l}(u|_{W_{2}})=0\cdot\partial_{l}(u|_{W_{2}})=0 on W2W_{2}, and by claim 1 of Restriction of a CkC^k Map to an Open Subset, lu=0\partial_{l}u=0 on W2W_{2}. Applying this to u=χu=\chi and then to u=iχu=\partial_{i}\chi (which is smooth, hence of class C1C^{1}, and vanishes on W2W_{2} by the first application), we get iχ=0\partial_{i}\chi=0 and jiχ=0\partial_{j}\partial_{i}\chi=0 on W2W_{2} for all i,j[q]i,j\in[q]. These functions are continuous on Rq\mathbb{R}^{q} (as χ\chi is of class C2C^{2}) and vanish whenever y>2\lVert y\rVert>2, so they are compactly supported by claim 2 of Compact Support on Rn\mathbb{R}^n Means Vanishing Outside a Bounded Set and bounded by claim 1 of A Continuous Compactly Supported Function on Rn\mathbb{R}^n is Bounded and Integrable. For i,j[q]i,j\in[q] choose bounds BiB_{i} and BjiB_{ji}, nonnegative real numbers by that definition, with iχ(y)Bi|\partial_{i}\chi(y)|\le B_{i} and jiχ(y)Bji|\partial_{j}\partial_{i}\chi(y)|\le B_{ji} for every yy, and put

M1=i=1qBi,M2=i=1q(j=1qBji),M_{1}=\sum_{i=1}^{q}B_{i},\qquad M_{2}=\sum_{i=1}^{q}\Bigl(\sum_{j=1}^{q}B_{ji}\Bigr),

finite sums of nonnegative real numbers. By claim 6 of Properties of Finite Sums (each summand of a sum of nonnegative terms is at most the sum, applied once for M1M_{1} and twice for M2M_{2}), BiM1B_{i}\le M_{1} and BjiM2B_{ji}\le M_{2} for all i,ji,j, and M1,M20M_{1},M_{2}\ge0 by claim 5 there.

Step 1: claim 1. Fix R>0R>0; R1>0R^{-1}>0 by claim 7 of Elementary Order Arithmetic in an Ordered Field, so R1=R1|R^{-1}|=R^{-1} by Absolute Value in an Ordered Field, and claim 5 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n gives R1x=R1x\lVert R^{-1}x\rVert=R^{-1}\lVert x\rVert for every xx. Multiplying by R1R^{-1}, respectively by RR, using claim 5 of Elementary Arithmetic in an Ordered Field for the weak inequalities and claim 10 of Elementary Order Arithmetic in an Ordered Field for the strict one, together with RR1=1R\,R^{-1}=1, we get for every xx:

xR    R1x1,x2R    R1x2,x>2R    R1x>2.\lVert x\rVert\le R\iff\lVert R^{-1}x\rVert\le1,\qquad \lVert x\rVert\ge2R\iff\lVert R^{-1}x\rVert\ge2,\qquad \lVert x\rVert>2R\iff\lVert R^{-1}x\rVert>2 .

Consequently 0χR10\le\chi_{R}\le1, χR(x)=1\chi_{R}(x)=1 whenever xR\lVert x\rVert\le R, χR(x)=0\chi_{R}(x)=0 whenever x2R\lVert x\rVert\ge2R, and χR\chi_{R} is compactly supported by claim 2 of Compact Support on Rn\mathbb{R}^n Means Vanishing Outside a Bounded Set.

Apply Partial Derivatives, Continuity and CkC^k Regularity under a Scaling Substitution with n=qn=q, m=1m=1, c=0Rqc=0_{\mathbb{R}^{q}}, λ=R1\lambda=R^{-1}, μ=1\mu=1, U=RqU=\mathbb{R}^{q} (open by claim 1 of Euclidean Space is Open in Itself, and CkC^k Maps are Continuous) and f=χf=\chi: since 0Rq+R1x=R1x0_{\mathbb{R}^{q}}+R^{-1}x=R^{-1}x (claim 1 of Euclidean Space Rn\mathbb{R}^n is a Real Vector Space), the function gg there is χR\chi_{R} and V=RqV=\mathbb{R}^{q}. By claim 5 there χR\chi_{R} is smooth, and by claim 2 there, for every xx and i[q]i\in[q],

iχR(x)=R1iχ(R1x).\partial_{i}\chi_{R}(x)=R^{-1}\,\partial_{i}\chi(R^{-1}x).

Apply the same lemma with the same c,λ,μ,Uc,\lambda,\mu,U to f=iχf=\partial_{i}\chi (smooth): the function gi(x)=iχ(R1x)g_{i}(x)=\partial_{i}\chi(R^{-1}x) has, by claim 2 there, jgi(x)=R1jiχ(R1x)\partial_{j}g_{i}(x)=R^{-1}\partial_{j}\partial_{i}\chi(R^{-1}x) for every xx and j[q]j\in[q]. Since iχR=R1gi\partial_{i}\chi_{R}=R^{-1}g_{i} on Rq\mathbb{R}^{q}, the scalar-multiple rule of claim 1 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set gives

jiχR(x)=R1jgi(x)=R2jiχ(R1x),\partial_{j}\partial_{i}\chi_{R}(x)=R^{-1}\,\partial_{j}g_{i}(x)=R^{-2}\,\partial_{j}\partial_{i}\chi(R^{-1}x),

where R2=R1R1R^{-2}=R^{-1}R^{-1}. By Step 0 and claim 4 of Properties of the Absolute Value in an Ordered Field, iχR(x)R1BiM1R1|\partial_{i}\chi_{R}(x)|\le R^{-1}B_{i}\le M_{1}R^{-1} and jiχR(x)R2BjiM2R2|\partial_{j}\partial_{i}\chi_{R}(x)|\le R^{-2}B_{ji}\le M_{2}R^{-2} (claim 5 of Elementary Arithmetic in an Ordered Field). This proves claim 1. We record for Step 3 that if x>2R\lVert x\rVert>2R then R1xW2R^{-1}x\in W_{2}, so by Step 0

χR(x)=0,iχR(x)=0,jiχR(x)=0(x>2R).\chi_{R}(x)=0,\qquad \partial_{i}\chi_{R}(x)=0,\qquad \partial_{j}\partial_{i}\chi_{R}(x)=0\qquad(\lVert x\rVert>2R).

Step 2: the function s(x)=12x2s(x)=\tfrac{1}{2}\lVert x\rVert^{2}. By claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, s(x)=12dE(x,0Rq)2s(x)=\tfrac{1}{2}\,d_{E}(x,0_{\mathbb{R}^{q}})^{2}, so A Scaled Squared Distance to a Point is of Class C2C^2, with Gradient and Hessian applies with n=qn=q, U=RqU=\mathbb{R}^{q}, a=0Rqa=0_{\mathbb{R}^{q}}, c=12c=\tfrac{1}{2} and its function qq taken to be ss: by its claim 1, js(x)=212(xj0)=xj\partial_{j}s(x)=2\cdot\tfrac{1}{2}\,(x_{j}-0)=x_{j}, that is js=πj\partial_{j}s=\pi_{j}; by its claim 2, ss is of class C2C^{2}; and by its claim 3, D2s(x)=(212)Iq=IqD^{2}s(x)=(2\cdot\tfrac{1}{2})I_{q}=I_{q} (the matrix scalar multiple being that of Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §background), so by Hessian Matrix of a C^2 Function, jis(x)=(Iq)ji=δji\partial_{j}\partial_{i}s(x)=(I_{q})_{ji}=\delta_{ji} for all i,j[q]i,j\in[q] and all xx. Moreover ss is smooth: xx2x\mapsto\lVert x\rVert^{2} is smooth by The Squared Euclidean Norm is Smooth, and ss is its scalar multiple by 12\tfrac{1}{2}, smooth by claim 3 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set.

Step 3: claim 2. Fix R>0R>0. As ψR=χRs\psi_{R}=\chi_{R}\,s is a product of smooth functions, it is smooth by claim 3 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set; it vanishes wherever χR\chi_{R} does, hence whenever x2R\lVert x\rVert\ge2R, so it is compactly supported by claim 2 of Compact Support on Rn\mathbb{R}^n Means Vanishing Outside a Bounded Set. By the product rule of claim 1 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set and Step 2, for all xx and i,j[q]i,j\in[q],

iψR(x)=iχR(x)s(x)+χR(x)xi,\partial_{i}\psi_{R}(x)=\partial_{i}\chi_{R}(x)\,s(x)+\chi_{R}(x)\,x_{i},

and, applying the sum and product rules of the same claim to this expression (whose two summands are products of functions of class C1C^{1}), with jπi=jis=δji\partial_{j}\pi_{i}=\partial_{j}\partial_{i}s=\delta_{ji} by Step 2,

jiψR(x)=jiχR(x)s(x)+iχR(x)xj+jχR(x)xi+χR(x)δji.\partial_{j}\partial_{i}\psi_{R}(x)=\partial_{j}\partial_{i}\chi_{R}(x)\,s(x)+\partial_{i}\chi_{R}(x)\,x_{j}+\partial_{j}\chi_{R}(x)\,x_{i}+\chi_{R}(x)\,\delta_{ji}.

Put M=2M2+4M1+1M=2M_{2}+4M_{1}+1, which does not depend on RR; since M1,M20M_{1},M_{2}\ge0 (Step 0) and 010\le1 (claim 1 of Elementary Arithmetic in an Ordered Field), claim 2 there gives 0M0\le M and M1+1MM_{1}+1\le M, and 0x0\le\lVert x\rVert for every xx by claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n. Fix xx and i,ji,j. If x>2R\lVert x\rVert>2R, all terms on the right of both displays vanish by Step 1, so iψR(x)=0\partial_{i}\psi_{R}(x)=0 and jiψR(x)=0\partial_{j}\partial_{i}\psi_{R}(x)=0, and the two bounds hold because their right sides are nonnegative (0Mx0\le M\lVert x\rVert by claim 5 of Elementary Arithmetic in an Ordered Field). If x2R\lVert x\rVert\le2R, then s(x)=12xx122Rx=Rxs(x)=\tfrac{1}{2}\lVert x\rVert\lVert x\rVert\le\tfrac{1}{2}\,2R\lVert x\rVert=R\lVert x\rVert and s(x)12(2R)2=2R2s(x)\le\tfrac{1}{2}(2R)^{2}=2R^{2} (claim 5 of Elementary Arithmetic in an Ordered Field and claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field), xi,xjx2R|x_{i}|,|x_{j}|\le\lVert x\rVert\le2R by claim 4 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, and χR(x)1|\chi_{R}(x)|\le1. Using claim 1, the multiplicativity and the triangle inequality of the absolute value (claims 4 and 5 of Properties of the Absolute Value in an Ordered Field) and claim 5 of Elementary Arithmetic in an Ordered Field,

iψR(x)M1R1Rx+x=(M1+1)xMx,|\partial_{i}\psi_{R}(x)|\le M_{1}R^{-1}\cdot R\lVert x\rVert+\lVert x\rVert=(M_{1}+1)\lVert x\rVert\le M\lVert x\rVert, jiψR(x)M2R22R2+M1R12R+M1R12R+1=2M2+4M1+1=M.|\partial_{j}\partial_{i}\psi_{R}(x)|\le M_{2}R^{-2}\cdot2R^{2}+M_{1}R^{-1}\cdot2R+M_{1}R^{-1}\cdot2R+1=2M_{2}+4M_{1}+1=M .

Finally, ΔψR(x)=i=1qiiψR(x)\Delta\psi_{R}(x)=\sum_{i=1}^{q}\partial_{i}\partial_{i}\psi_{R}(x) satisfies ΔψR(x)i=1qiiψR(x)|\Delta\psi_{R}(x)|\le\sum_{i=1}^{q}|\partial_{i}\partial_{i}\psi_{R}(x)| by claim 2 of Comparison and Absolute Value Bounds for Finite Sums of Real Numbers, and i=1qiiψR(x)i=1qM\sum_{i=1}^{q}|\partial_{i}\partial_{i}\psi_{R}(x)|\le\sum_{i=1}^{q}M by claim 1 of the same lemma; and i=1qM=Mι(q)=qM\sum_{i=1}^{q}M=M\,\iota(q)=qM by claim 3 of Properties of Finite Sums and The Canonical Map from the Natural Numbers to a Field. This proves claim 2.

Step 4: claim 3. Fix R>0R>0 and let B={yRq:y<R}B=\{y\in\mathbb{R}^{q}:\lVert y\rVert<R\}. The set BB is open: if yBy\in B and yy<Ry\lVert y'-y\rVert<R-\lVert y\rVert, then yy+yy<R\lVert y'\rVert\le\lVert y\rVert+\lVert y'-y\rVert<R by claim 6 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n applied to y=y+(yy)y'=y+(y'-y), so the argument of Step 0 applies. By Step 1, χR(y)=1\chi_{R}(y)=1 for every yBy\in B, so ψR(y)=s(y)\psi_{R}(y)=s(y) for every yBy\in B; that is, ψRB=sB\psi_{R}|_{B}=s|_{B}. Let xBx\in B and i,j[q]i,j\in[q]. By claim 1 of Restriction of a CkC^k Map to an Open Subset applied to ψR\psi_{R} and to ss (both of class C1C^{1} on Rq\mathbb{R}^{q}),

iψR(x)=i(ψRB)(x)=i(sB)(x)=is(x)=xi,\partial_{i}\psi_{R}(x)=\partial_{i}(\psi_{R}|_{B})(x)=\partial_{i}(s|_{B})(x)=\partial_{i}s(x)=x_{i},

the last equality by Step 2. Since this holds at every point of BB, the functions iψR\partial_{i}\psi_{R} and is\partial_{i}s (both of class C1C^{1} on Rq\mathbb{R}^{q}, as ψR\psi_{R} and ss are of class C2C^{2}) have the same restriction to BB, and the same claim 1 gives jiψR(x)=jis(x)=δji=δij\partial_{j}\partial_{i}\psi_{R}(x)=\partial_{j}\partial_{i}s(x)=\delta_{ji}=\delta_{ij}. Hence ΔψR(x)=i=1qδii=i=1q1=ι(q)=q\Delta\psi_{R}(x)=\sum_{i=1}^{q}\delta_{ii}=\sum_{i=1}^{q}1=\iota(q)=q by The Canonical Map from the Natural Numbers to a Field, and ψR(x)=s(x)=12x2\psi_{R}(x)=s(x)=\tfrac{1}{2}\lVert x\rVert^{2}. This proves claim 3.

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